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NSR database version of May 10, 2024.

Search: Author = K.M.Murray

Found 5 matches.

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1971MU11      Lett.Nuovo Cim. 1, 571 (1971)

K.M.Murray, M.E.Toms

13C Giant Resonance and Excited States of the Residual Nuclei

NUCLEAR REACTIONS 13C(γ, nγ), E < 21, 28 MeV; measured σ(E;Eγ). 13C deduced giant resonance structure.

doi: 10.1007/BF02770151
Citations: PlumX Metrics


1970HA28      Phys.Rev. C2, 761 (1970)

E.Hayward, R.B.Schwartz, K.M.Murray

Comments on 'Isospin of the B11 Giant Resonance'

NUCLEAR REACTIONS 11B(γ, Xγ), E not given; measured nothing; reinterpreted data. 11B deduced nothing on T-splitting of giant resonance.

doi: 10.1103/PhysRevC.2.761
Citations: PlumX Metrics


1969MU07      Phys.Rev. 182, 1097 (1969)

K.M.Murray, J.C.Ritter

O16(γ, n)O15* and O16(γ, p)N15* Reactions and the Electromagnetic Decay of O15* and N15*

NUCLEAR REACTIONS 16O(γ, nγ), (γ, pγ), E < 30 MeV; measured σ(E;Eγ), Doppler shift. 15N, 15O deduced levels, T1/2, level-width, γ-branching. Ge(Li) detector.

doi: 10.1103/PhysRev.182.1097
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1969MU10      Phys.Rev.Letters 23, 1461 (1969)

K.M.Murray

Isospin of the B11 Giant Resonance

NUCLEAR REACTIONS 11B(γ, nγ), (γ, pγ), E < 24, 35 MeV; measured σ(E;Eγ). 11B deduced no T=3/2 giant resonance.

doi: 10.1103/PhysRevLett.23.1461
Citations: PlumX Metrics


1963MU08      Phys.Rev. 132, 1134 (1963)

K.M.Murray, W.L.Bendel

Photoprotons from C12 and F19

NUCLEAR STRUCTURE 12C, 19F; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.132.1134
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